Dynamical Selection of Critical Exponents

In renormalized field theories there are in general one or few fixed points which are accessible by the renormalization-group flow. They can be identified from the fixed-point equations. Exceptionally, an infinite family of fixed points exists, parameterized by a scaling exponent $\zeta$, itself function of a non-renormalizing parameter. Here we report a different scenario with an infinite family of fixed points of which seemingly only one is chosen by the renormalization-group flow. This dynamical selection takes place in systems with an attractive interaction $\mathcal{V}(\varphi )$, as in standard ${\varphi }^4$ theory, but where the potential $\mathcal{V}$ at large $\varphi$ goes to zero, as e.g. the attraction by a defect.